DC—DC converter and device for operation of a high pressure discharge lamp using said converter

ABSTRACT

A DC-DC converter which accomplishes a reduction of the switching loss in the wide, variable range of the continuity ratio of the main switching device includes a direct current source, an ON-OFF-controllable main switching device, a main coil which is series connected to the main switching device, a fly-wheel diode which is arranged such that the induction current of the above described main coil flows when the main switching device is shifted into the OFF state, a smoothing capacitor for smoothing the output of the main coil, an auxiliary coil, a resonant capacitor and an ON-OFF-controllable auxiliary switching device, in which the auxiliary coil and the resonant capacitor are series-connected to form a LC series connection. Further, the LC series connection, the main switching device and the fly-wheel diode are also series connected, with the auxiliary switching device being connected in parallel to the LC series connection.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The invention relates to a DC-DC converter of the voltage reduction-buck type with the PWM (pulse width modulation) method in which the efficiency is increased, and a device for using a DC-DC converter to operate a high pressure discharge lamp such as a metal halide lamp, mercury lamp or the like.

2. Description of the Related Art

Conventionally, of the converters that convert the voltage of a DC source into another value, output it and supply it to a load, i.e. DC-DC converters, the converter of the voltage reduction-buck type, which is shown in FIG. 15, is often used to carry out voltage reduction-conversion.

In this circuit, the current from the DC source (Vin) is repeatedly shifted by a main switching device (Qx′) such as a FET or the like into the ON state or the OFF state, and a smoothing capacitor (Cx′) is charged via the main coil (Lx′). In this arrangement, this voltage can be applied to a load (Zx).

During the interval in which the above described main switching device (Qx′) is in the ON state, charging of the smoothing capacitor (Cx′) and current supply to the load (Zx) are carried out directly by the current through the main switching device (Qx′), and moreover in the main coil (Lx′), energy is stored in the form of a flux. During the interval in which the main switching device (Qx′) is in the OFF state, the smoothing capacitor (Cx′) is charged via a fly-wheel diode (Dx′) by the energy stored in the form of a flux in the main coil (Lx′) and current is supplied to the load (Zx).

This converter is operated under PWM control of the main switching device (Qx′). Specifically, by feedback control of the ratio between the time interval in the ON state and the sum of the period of the ON state and the period of the OFF state of the main switching device (Qx′), i.e. the continuity ratio, the voltage supplied to the load (Zx) can be adjusted, even as the voltage of the DC source (Vin) fluctuates, to a desired (for example, constant) value, the supplied current can be adjusted to a desired value and the supplied wattage can be adjusted to the desired value.

Of course, the value of the desired efficiency (voltage, current, wattage or the like) can assume a constant value or it can also be changed over time. For feedback control of the desired efficiency, a detector is needed to determine the output voltage and the output current, as is a feedback control circuit, which is not shown in the drawings.

FIG. 16 shows the voltage and current waveform of this converter using one example. If the main switching device (Qx′) is shifted into the ON state, the voltage (VxD′) supplied to the main switching device (Qx′) passes from the voltage of the DC source (Vin) essentially to 0 V. However, this transition does not take place instantaneously, but requires a certain time.

Here, in the process in which the voltage (VxD′) of the main switching device (Qx′) gradually decreases, the current (IQx′) of the main switching device (Qx′) also gradually begins to flow. There is therefore an interval during which neither the voltage (VxD′) nor the current (IQx′) is 0. According to the size of the time integral of the product of the voltage and the current, for each transition of the main switching device (Qx′) into the ON state a switching loss (SwL) occurs on the main switching device (Qx′).

This switching loss also arises by the same process in the case of the transition into the ON state as in a transition into the OFF state. But normally the loss in the transition into the ON state is greater. The reason is that, when the main switching device (Qx′) is a FET, for example, a parasitic electrostatic capacitance is present between the source electrode and the drain, that the electrical charge which has been charged onto this electrostatic capacitance during the interval of the OFF state of the main switching device (Qx′) at the voltage of the DC source (Vin), in the transition into the ON state is subjected to forced short circuit discharge, and that the energy which is consumed in doing so is added to the switching loss (SwL).

When this switching loss is present, there is not only the disadvantage of a reduction in the efficiency of the converter, but also the disadvantage of a large converter and a cost increase of it, since the heat generation of the main switching device (Qx′) is large and since therefore a switching device with large maximum power dissipation must be used and there must be a large radiator with high radiation efficiency in addition. Furthermore, the fan that supplies cooling air for cooling the radiator must be a high capacity fan, which brings the disadvantages of the reduction in the efficiency and the increase in size and cost of the converter.

In order to eliminate these disadvantages, conventionally a host of proposals have been made. They are mainly technologies that prevent intervals during which neither the voltage (V×D′) nor the current (IQx′) is 0. Normally the technology in which switching is carried out at a 0 voltage of the switching device, is called zero voltage switching, and the technology in which switching is carried out at a 0 current of the switching device, is called zero current switching. Often, using a so-called LC resonance the voltage applied to the switching device and the current flowing in the switching device are temporarily taken over by the voltage induced by the L component (coil) and the current flowing in the C component (capacitor) and are essentially set or reduced to 0, and during this time a transition of the switching device into the ON state or the OFF state is carried out.

For example, in Japanese patent disclosure document HEI 1-218352 a DC-DC converter of the voltage reduction-buck type with current resonance is proposed. In this proposal the current flowing in the main switching device (Qx′), however, due to resonance has a higher peak value than a conventional DC-DC converter of the voltage reduction-buck type. Therefore, it becomes necessary to use a switching device with a high current. Furthermore, in the case in which the switching frequency is higher than the resonant frequency, it is possible that the loss continues to increase because the switching device is shifted into the OFF state at a high current.

Additionally, in this circuit arrangement, according to the assumption of a constant output voltage for a DC-DC converter, the PWM method is undertaken with a constant switching frequency. Because of this, it is necessary to match the continuity ratio thereof to the resonant frequency. The range of the continuity ratio is therefore limited. An increase of the efficiency can therefore only be accomplished in the vicinity of the rated output voltage. Neither a guideline nor conditions for a measure against the fluctuation of the load were considered.

Furthermore, for example, U.S. Pat. No. 5,880,940 discloses a DC-DC converter of the voltage reduction-buck type in which a secondary winding is added to the main coil (Lx′), and thus, a transformer is formed.

In this proposal, a DC-DC converter is described as being operated by connecting an auxiliary switching device to the transformer as a forward converter. However, an increase of the ripple in the output current by this operation was not even considered. The added auxiliary switching device cannot be subjected to zero voltage switching either. It is necessary to add another coil and to carry out zero current switching.

In the case of zero current switching, different from zero voltage switching, there is specifically the disadvantage that the problem of power consumption loss as a result of the forced short circuit discharge is not eliminated in the transition of the electrical charge into an ON state which was charged in the parasitic electrostatic capacitance of the main switching device. Therefore, this is not ideal.

On the other hand, if the use of a DC-DC converter of the voltage reduction-buck type is considered, the resonant conditions of the LC resonance circuit are easily satisfied in a stable manner, since the output voltage is relatively stable for applications such as a constant voltage current source or the like.

However, in the case of use as a device for operating a high pressure discharge lamp, such as a metal halide lamp, a mercury lamp or the like, the lamp voltage as the output voltage is changed significantly by the state of the lamp as a load. Under certain circumstances it fluctuates steeply. Therefore, a specially adapted construction is needed. The converter must also be matched to this construction.

The feature of the high pressure discharge lamp as the load of the converter is described below. Generally a high pressure discharge lamp (Ld) has an arrangement in which a discharge space (Sd) is filled with a discharge medium which contains mercury and in which a pair of electrodes (E1, E2) is located oppositely for the main discharge. Between the electrodes (E1, E2) an arc discharge is produced and the radiation emitted from the arc plasmas is used as the light source.

The high pressure discharge lamp (Ld), different from a general load, exhibits a property which is closer to a Zener diode than to an impedance element. This means that the lamp voltage does not change greatly, even if the flowing current changes. A lamp voltage which corresponds to a Zener voltage however changes greatly depending on the discharge state.

Specifically, in the state before the start of the discharge, the Zener voltage is extremely high because no current at all is flowing. If, by operating a starter, such as a high voltage pulse generator or the like, a discharge is started, a glow discharge is formed. In the case, for example, of a discharge lamp which contains greater than or equal to 0.15 mg of mercury per cubic millimeter of volume of the discharge space (Sd), the glow discharge voltage ranges from 180 V to 250 V. In the state before the start of the discharge, a voltage of at least equal to the glow discharge voltage is applied to the high pressure discharge lamp. Normally, this voltage is roughly 270 V to 350 V and is called the no-load voltage. The starter is operated in this way.

When the electrodes (E1, E2) are heated by the glow discharge to a sufficient degree, a sudden transition into an arc discharge takes place. Immediately after the transition a low arc discharge voltage from 8 V to 15 V is shown. This is a transient arc discharge. The arc discharge vaporizes the mercury and if heating of the mercury vapor continues, the arc discharge voltage gradually increases until it reaches a steady-state arc discharge from 50 V to 150 V. The voltage in a steady-state arc discharge, i.e., the lamp voltage, depends on the density of the mercury which has been added to the discharge space (Sd) and the distance between the electrodes (E1, E2).

Immediately after the transition into the arc discharge, depending on the vapor state of the mercury, the glow discharge suddenly returns or the arc discharge and the glow discharge takes place alternately in a vigorous back and forth manner.

At a constant voltage from the DC source (Vin) the output voltage of the DC-DC converter of the voltage reduction-buck type is at a value which is obtained by multiplying roughly the voltage of the DC source (Vin) by the continuity ratio. Therefore, the DC-DC converter of the voltage reduction-buck type can be kept approximately for the DC-constant voltage current source.

On the other hand, in idealized switching theory, in the case in which a DC-constant voltage current source is connected to a Zener diode as a load, i.e., still another DC-constant voltage current source, the theory fails and good analysis is not possible. More accurately, when in the case of connecting a Zener diode as the load to a constant voltage current source, the output voltage of the constant voltage current source is lower than the Zener voltage, no current at all flows in the Zener diode. Conversely, in the case in which the output voltage of the constant voltage current source is higher than the Zener voltage, an infinitely large current flows.

In the case in which a discharge lamp which can be roughly regarded as a Zener diode is connected to a realistically present DC-DC converter of the voltage reduction-buck type as a load, extinction of the discharge occurs in the case in which the output voltage of the converter is lower than the Zener voltage. Conversely, in the case in which the output voltage of the converter is higher than the Zener voltage, an unduly high current which is determined by the current serviceability of the DC source (Vin) and of the converter flows in the lamp.

Therefore, in a device for operating a high pressure discharge lamp, the following is required of a converter for supplying a high pressure discharge lamp:

There is a demand for the property which enables a prompt change of the continuity ratio in a wide, variable range for PWM control according to the discharge voltage of the high pressure discharge lamp in order to prevent extinction of the discharge from occurring or an unduly large current from flowing and the lamp and converter circuit from being damaged. These must be achieved even at a discharge voltage that corresponds to the no-load voltage which changes in this way to a great extent and also vigorously depends on the discharge state, i.e., the state in which a no-load voltage is applied (state before the start of discharge), the glow discharge state, the state of a transient arc discharge, or the steady-state arc discharge state. Furthermore there is a demand for a property that enables maintenance of operation in which the switching loss is reduced by resonant operation.

In the case of high ripple which is contained in the current flowing in the discharge lamp, there is a case in which instability, flicker and extinction of the discharge arise due to acoustic resonance. Therefore, it is required of the converter that the ripple of the output current is small. As a result, it is necessary to prevent the operation of the resonant circuit which is arranged for reducing switching loss from accelerating the formation of a superfluous ripple component.

In the case, for example, of a DC-DC converter of the voltage reduction-buck type which is described in the above cited U.S. Pat. No. 5,880,940, the main coil also acts as a transformer with a resonant oscillation effect. Originally during the interval in which the main switching device is in the ON state, in base operation of the DC-DC converter of the voltage reduction-buck type on its two ends the main coil has a difference voltage between the supplied DC source voltage and the output voltage and works in such a way that the input DC source voltage is not applied directly to the load.

In the case of a great fluctuation of the output voltage, of course, the voltage on the primary side of the transformer fluctuates greatly with a resonant oscillation effect. Since the energy transmitted to the secondary circuit of the transformer also fluctuates greatly because of the resonant oscillation effect, as a result the resonant operation also fluctuates greatly. The DC-DC converter of the voltage reduction-buck type described in U.S. Pat. No. 5,880,940 is therefore not suited as a converter for supplying a high pressure discharge lamp.

As was mentioned above, it is necessary in a DC-DC converter of the voltage reduction-buck type to reduce the switching loss in order to avoid raising the size and costs of the converter. But in the prior art it was difficult to have a wide, variable range of output voltage and keep down the cost because of the addition of the resonant circuit. In particular it was difficult to obtain a converter that is suited to operate a high pressure discharge lamp.

SUMMARY OF THE INVENTION

A primary object of the present invention is to devise a DC-DC converter that eliminates the disadvantage of a conventional DC-DC converter, i.e., the disadvantage of difficult implementation of a reduction of the switching loss in a wide, variable range of the continuity ratio of the main switching device with low costs.

Another object of the invention is to devise a device for operating a high pressure discharge lamp that eliminates the disadvantage of a conventional device for operating a high pressure discharge lamp, i.e., the disadvantage of difficult implementation of a reduction of the switching loss with low costs.

According to a first aspect of the invention, for a DC-DC converter of the voltage reduction-buck type which comprises the following:

-   -   a direct current source (Vin);     -   an ON-OFF-controllable main switching device (Qx);     -   a main coil (Lx) which is series connected to the main switching         device (Qx);     -   a fly-wheel diode (Dx) which is arranged such that the induction         current of the above described main coil (Lx) flows when the         main switching device (Qx) is shifted into the OFF state; and     -   a smoothing capacitor (Cx) for smoothing the output of the main         coil (Lx), the object is achieved in that furthermore there are         an auxiliary coil (Lw), a resonant capacitor (Cw) and an         ON-OFF-controllable auxiliary switching device (Qw), that the         auxiliary coil (Lw) and the resonant capacitor (Cw) are         series-connected and thus form a LC series connection, that this         LC series connection, the main switching device (Qx) and the         fly-wheel diode (Dx) are series connected, that the auxiliary         switching device (Qw) is connected in parallel to the LC series         connection, and that the main switching device (Qx) and the         auxiliary switching device (Qw) are controlled such that they         are shifted in alternation into the ON state and moreover the         main switching device (Qx), after the auxiliary switching device         (Qw) has been shifted into the OFF state, is shifted into the ON         state within a given time.

According to one development of the above described invention, these objects are achieved by the following operations: in the state in which the resonance prohibition signal (Sc) is activated, the auxiliary switching device (Qw) is shifted into the ON state when the ON state of the main switching device (Qx) is reached, instead of being shifted into the ON state alternately with the main switching device (Qx); and the main switching device (Qx) is shifted into the ON state within a given time after the auxiliary switching device (Qw) has been shifted into the OFF state.

According to a second aspect of the invention, in a device for operating a high pressure discharge lamp (Ld) in which the discharge space (Sd) is filled with a discharge medium and there is a pair of opposed electrodes (E1, E2) for the main discharge, the objects are achieved in that the DC-DC converter described above is used for supplying the high pressure discharge lamp (Ld).

Advantages

First of all, the action of the invention is described in its first aspect.

In this invention, by the arrangement of the DC-DC converter which is described in achieving the object, the auxiliary switching device (Qw) is shifted into the OFF state before the main switching device (Qx) is shifted into the ON state, furthermore in the auxiliary coil (Lw) a voltage is induced in the direction in which the main switching device (Qx) is biased in the backward direction, and the electrical charge of the parasitic electrostatic capacitance of the main switching device (Qx) is discharged via a fly-wheel diode (Dx). In this way, the invention acts such that zero voltage switching is obtained when the main switching device (Qx) is shifted into the ON state. Details are given below.

Furthermore, as is described below, because control is exercised such that the auxiliary switching device (Qw) is shifted into the ON state within a given time after the main switching device (Qx) has been shifted into the OFF state, the following can be achieved.

Before the auxiliary switching device (Qw) is shifted into the ON state, the main switching device (Qx) is shifted into the OFF state, in the auxiliary coil (Lw) the voltage is induced in the direction in which the auxiliary switching device (Qw) is biased in the backward direction and the electrical charge of the parasitic electrostatic capacitance of the auxiliary switching device (Qw) is discharged. In this way zero voltage switching can be obtained when the auxiliary switching device (Qw) is shifted into the ON state.

The invention is further described below using several embodiments which are shown in the drawings.

BRIEF DESCRIPTION OF THE DRAWINGS

FIG. 1 shows a schematic of the circuit arrangement of a DC-DC converter according to the first aspect of the invention;

FIG. 2 shows a schematic of the voltages and the current waveforms which correspond to the circuit arrangement of the DC-DC converter according to the first aspect of the invention;

FIG. 3 shows a schematic of the timing of driving of the main switching device and the auxiliary switching device according to a development of the first aspect of the invention;

FIG. 4 shows a schematic of the timing of driving of the main switching device and the auxiliary switching device according to a development of the first aspect of the invention;

FIG. 5 shows a schematic of the circuit arrangement of a DC-DC converter according to the second aspect of the invention;

FIG. 6 shows a schematic of another embodiment of the invention according to the first aspect of the invention;

FIG. 7 shows a schematic of another embodiment of the invention according to the first aspect of the invention;

FIG. 8 shows a schematic of the arrangement of a driver control element (Gw) and a feedback control element (Fb) of the DC-DC converter of the invention;

FIG. 9 shows a schematic of one embodiment of the circuit arrangement of the driver control element (Gw) and of part of the feedback control element (Fb) of a DC-DC converter of the invention;

FIG. 10 shows a schematic of one embodiment according to the second aspect of the invention;

FIG. 11 shows a schematic of another embodiment according to the second aspect of the invention;

FIG. 12 shows a schematic of one embodiment of the control sequence of the third aspect of the invention;

FIG. 13 shows a schematic of one embodiment according to the third aspect of the invention;

FIG. 14 shows a schematic of the voltages measured in reality and of current waveforms of the DC-DC converter according to the third aspect of the invention;

FIG. 15 shows a schematic of the circuit arrangement of a conventional DC-DC converter of the voltage reduction-buck type; and

FIG. 16 shows a schematic of the voltages and of the current waveforms of the circuit arrangement of a conventional DC-DC converter of the voltage reduction type.

DETAILED DESCRIPTION OF THE INVENTION

FIG. 1 shows the arrangement of the circuit of a DC-DC converter of the invention in a simplified representation. FIG. 2 shows essentially the respective waveform in the circuit shown in FIG. 1.

This circuit has the same arrangement as in the conventional DC-DC converter of the voltage reduction-buck type, in which the following takes place:

-   -   during the interval in which the main switching device (Qx)         which consists of a FET or the like is in the ON state, a         current flows from the DC source (Vin) via the main coil (Lx)         which is series connected to the main switching device (Qx).         Here furthermore the smoothing capacitor (Cx) of the main coil         (Lx) which is connected to the terminal opposite the main         switching device (Qx) is charged, current is supplied to the         load (Zx) which is connected in parallel to the smoothing         capacitor (Cx) and moreover energy in the form of a flux is         stored in the main coil (Lx). During the interval in which the         main switching device (Qx) is in the OFF state, the smoothing         capacitor (Cx) is charged by the energy stored in the main coil         (Lx) in the form of a flux via the fly-wheel diode (Dx) in which         a cathode is connected to one node between the main switching         device (Qx) and the main coil (Lc) and current is supplied to         the load (Zx).

In this circuit arrangement, in addition to the same arrangement as the arrangement of the conventional DC-DC converter of the voltage reduction-buck type, the following actions are implemented:

-   -   the auxiliary coil (Lw) and the resonant capacitor (Cw) are         series connected and thus a LC series connection is formed;     -   This LC series connection is connected such that the DC source         (Vin), the main switching device (Qx) and the fly-wheel diode         (Dx) are series connected; and     -   The auxiliary switching device (Qw) is connected in parallel to         the LC series connection.

Here, the basic principle is that the main switching device (Qx) and the auxiliary switching device (Qw) are operated such that one of the two is shifted into the OFF state when the other is in the ON state. However, control is exercised such that the auxiliary switching device (Qw) is shifted beforehand into the OFF state by a switch closing prohibition interval (τy), which is described below, before the main switching device (Qx) is shifted into the ON state.

During the interval shown in FIG. 2, from a time (t1) until a time (t2) is reached, the main switching device (Qx) is in the ON state. However, the auxiliary switching device (Qw) is in the OFF state. Current supply from the DC source (Vin) to the load side is therefore carried out via the auxiliary coil (Lw) and the resonant capacitor (Cw). This means that current supply is carried out as the resonant current of the LC series connection. The resonant phenomenon here is a LC resonance by the inductance of the auxiliary coil (Lw) and the resonant capacitor (Cw).

During the interval from the time (t1) until the time (t2) is reached, the resonant capacitor (Cw) is charged, resulting in a voltage that is gradually reduced and applied to one terminal on the input side of the main coil (Lx). To prevent this amount of reduction of the voltage from becoming too large by the time the interval (Ton) ends and the capacity for current feed to the switching parts starting with the main coil (Lx) from being additionally reduced, it is advantageous for the resonant capacitor (Cw) to have electrostatic capacitance in a sufficient amount, considering the switching frequency of this circuit.

During this interval, the resonant capacitor is charged and electrical energy is stored. In doing so the current flows in the auxiliary coil (Lw) and magnetic energy is stored in it. This means that resonant energy is stored in the LC series connection. This energy is consumed in order to later carry out resonant operation.

If next, at the time (t2), the main switching device (Qx) is shifted into the OFF state, as is described below, the voltage between the terminals of the auxiliary switching device (Qw) passes into a low state, so that the voltage of the DC source (Vin) is applied to the main switching device (Qx). Therefore, in the parasitic electrostatic capacitance of the main switching device (Qx), the electric charge is charged up to this voltage.

Since at the same time (t2) energy is stored in the LC series connection, in the closed loop comprised of the auxiliary coil (Lw), the resonant capacitor (Cw) and the auxiliary switching device (Qw), the resonant current flows without interruption. With respect to the auxiliary switching device (Qw), the current begins to flow, however, via an antiparallel diode (Dqw) which is connected in parallel thereto.

The antiparallel diode (Dqw) is present as an outside element, for example, in the case in which the auxiliary switching device (Qw) is a MOSFET. It can also be used as such.

With respect to the timing for turning on the auxiliary switching device (Qw), it is advantageous to shift as quickly as possible the auxiliary switching device (Qw) into the ON state while ensuring enough time to prevent this timing from coinciding with the ON interval of the main switching device (Qx) before the main switching device (Qx) is shifted into the OFF state. The reason for this is that during the interval in which current is flowing in the antiparallel diode (Dqw), a forward voltage of the antiparallel diode (Dqw) forms and that if in doing so the auxiliary switching device (Qw) is in the ON state, the forward voltage of the antiparallel diode (Dqw) can be reduced. By the same principle as in the case of a so-called synchronous rectification the loss in the above described antiparallel diode (Dqw) and in the auxiliary switching device (Qw) can be reduced. This is one of the advantages of the invention.

Since the peak value of the resonant voltage applied to the resonance capacitor (Cw) changes with the different constants of the components comprising the circuit, combinations of different constants can be used in conjunction with the maximum ratings of the components used and the costs are advantageous.

The peak value of the voltage applied to the resonant capacitor (Cw) is essentially proportional to the output wattage of the DC-DC converter of the voltage reduction-buck type. For example, for constant power regulation the peak value of the voltage applied to the resonant capacitor (Cw) is essentially constant. In the case of a small output voltage the peak value of the voltage applied to the resonant capacitor (Cw) is reduced, which raises the possibility that resonant operation does not take place to a sufficient degree. But since the output wattage is small, and since thus originally the switching loss is also small, of the invention, this is not regarded as disadvantageous. Therefore, to carry out resonant operation under the condition which is similar to the maximum utilization output wattage, the different constants of the components comprising the circuit can be adjusted.

In the circuit arrangement of the invention, by the measure that there are an auxiliary coil (Lw) and a resonant capacitor (Cw) which are independent of the basic (conventional) DC-DC converter part of the voltage reduction-buck type, and that resonant operation is carried out, a reduction of the switching loss is desired. Therefore the different constants of the switching devices comprising the resonant circuit, i.e., the parameters of the resonant circuit, can be adjusted essentially independently.

Therefore, it is possible to perform operations such as intentionally setting the inductance of the auxiliary coil (Lw) to be smaller than the inductance of the main coil (Lx) and still achieving good resonant operation. This measure of the invention results in that even under the conditions when the output voltage changes greatly, as in the case in which the high pressure discharge lamp is used as a load, basic operation of the DC-DC converter part of the voltage reduction-buck type is fixed, depending largely only on the inductance of the main coil (Lx) when the resonant capacitor has a large enough capacitance.

On the other hand, since the auxiliary coil (Lw) is located in the path through which energy is supplied to the basic DC-DC converter part of the voltage reduction-buck type, the magnetic energy stored in the auxiliary coil (Lw) during the interval of the ON state of the main switching device (Qx) is essentially proportional to the energy supplied to the load during each period of switching operation. This relation hardly depends on the voltage applied to the load.

Therefore, when the wattage supplied to the load does not change greatly, the voltage charged in the resonant capacitor (Cw) does not change greatly under the conditions under which the output voltage changes greatly. The resonance phenomenon in the main coil (Lw), which has an intentionally smaller inductance than the main coil (Lx), therefore becomes difficult to be influenced by the fluctuation of conditions for the load. This feature is one of the major advantages of the invention.

At the time (t3), which is shown in FIG. 2, the resonant voltage of the resonant capacitor (Cw) reaches a peak value, and the resonant current flowing in the auxiliary coil (Lw) reaches 0 and then begins to flow in the direction opposite the previous direction. As was described above, it becomes apparent that zero voltage switching is achieved when the transition of the above described auxiliary switching device (Qw) into the ON state is completed within an interval (τx) which begins at the time (t2), which is prior to the time (t3) and at which the main switching device (Qx) is shifted into the OFF state. Furthermore, during the interval, current is flowing in the antiparallel diode (Dqw) and only the forward voltage of the antiparallel diode (Dqw) is formed for the voltage of the auxiliary switching device (Qw).

This means that by setting the timing of shifting the auxiliary switching device (Qw) into the ON state to be shorter than the length of time of τxx of the interval (τx) such that enough time is ensured to prevent this timing from coinciding with the ON interval of the main switching device (Qx), the switching loss can also be kept low during the switching operation of the auxiliary switching device (Qw). This is one of the major advantages of the invention.

As was described above, generally, control is exercised such that, before the main switching device (Qx) reaches the ON state at the time (t4) shown in FIG. 2, the auxiliary switching device (Qw) is shifted into the OFF state by a switch closing prohibition interval (τy).

As was described above, at the time (t2), within the interval during which the forward current is flowing in the main switching device (Qx), the main switching device (Qx) is shifted into the OFF state, and the current of the auxiliary coil (Lw) is continued. In this way, current flows in the closed loop comprised of the auxiliary coil (Lw), the above described resonant capacitor (Cw) and the antiparallel diode (Dqw) of the auxiliary switching device (Qw). In the same way, this time, in the line path which passes through the region in which the main switching device (Qx) is present and located outside of the closed loop, current begins to flow in such a way that the current of the auxiliary coil (Lw) is continued when the auxiliary switching device (Qw) reaches the OFF state at the time (t4).

However, in this case, since the direction of the current of the auxiliary coil (Lw) which continues to try to flow is opposite that at the time (t2), the current also begins to flow in the line path which passes through the area in which the main switching device (Qx) is present in the opposite direction, i.e., in the direction in which the backward current flows in the main switching device (Qx). This means that current begins to flow via the line path consisting of the above described auxiliary coil (Lw), the fly-wheel diode (Dx) and the antiparallel diode (Dqx) which is connected parallel to the main switching device (Qx), from the grounding terminal of the DC source (Vin) to the positive terminal.

Here, the electrical charge which is charged in the parasitic electrostatic capacitance of the main switching device (Qx) is withdrawn. Afterwards, during the interval in which in the antiparallel diode (Dqx) current is flowing, a state is maintained on the two ends of the main switching device (Qx) in which only a forward voltage of the antiparallel diode (Dqx) is formed.

The antiparallel diode (Dqw) is present as an outside element, for example, in the case in which the auxiliary switching device (Qw) is a MOSFET. It can also be used as such.

The phenomenon that, by operation at time (t4), current flows from the grounding terminal of the DC source (Vin) to the positive terminal means that the energy of resonance operation which has been stored in the auxiliary coil (Lw) is regenerated in the DC source (Vin) and one of the major advantages of the invention is that energy is not wasted.

As was described above, the main switching device (Qx) is shifted into the ON state at the time (t5) shown in FIG. 2 after expiration of the switch closing prohibition interval (τy), which starts when the auxiliary switching device (Qw) reaches the OFF state. This is completed within an interval with a state in which in the antiparallel diode (Dqx) current is flowing and in which on the two ends of the main switching device (Qx) only the forward voltage of the antiparallel diode (Dqx) forms.

By this measure, the current flowing in the antiparallel diode (Dqx) finally reaches 0 at the time (t6) shown in FIG. 2. Zero voltage switching can be achieved when the current is next inverted and flows in the forward direction of the main switching device (Qx). This means that, in the main switching device's (Qx's) transition into the ON state, the switching loss can be kept low and the advantage of the invention can be exploited.

FIG. 2 shows the interval (τz) from the time (t4) at which the auxiliary switching device (Qw) is shifted into the OFF state until the time (t6) at which the current flowing in the antiparallel diode (Dqx) reaches 0. The interval is depicted in the figure as relatively long for the ease of drawing. In actual switching operation, the interval (τz) is a short interval since the parasitic electrostatic capacitance of the main switching device (Qx) is normally a few pF to a few dozen pF, therefore is small.

During the switch closing prohibition interval (τy), it is necessary to set the timing by which the auxiliary switching device (Qx) is shifted into the ON state to be shorter than the length of time of τZZ of the interval (τz) such that enough time is ensured to prevent this timing from coinciding with the ON interval of the above described main switching device (Qx). When this condition is satisfied, the switch closing prohibition interval (τy) can be set to be constant or can be changed depending on conditions.

As was described above, according to the first aspect of the invention, the switching loss can be reduced in the transition operation of the main switching device (Qx) into the ON state. The auxiliary coil (Lw) is arranged independently of the circuit arrangement of the basic DC-DC converter of the voltage reduction-buck type. Because the inductance of the auxiliary coil (Lw) is intentionally set to be smaller than the inductance of the main coil (Lx), and because the resonant capacitor is set to be great, the resonance phenomenon for the auxiliary coil (Lw) becomes less susceptible to the fluctuation of conditions at the load. Therefore, in a wide, variable range of the continuity ratio of the main switching device, the switching loss can be reduced.

Furthermore, if the parameters of the auxiliary coil (Lw) and of the resonant capacitor (Cw) are set in a suitable manner hereby, the switching loss can be reduced in transition operation of the auxiliary switching device (Qw) into the ON state. Also, the energy of the resonant operation of the auxiliary coil (Lw) in the DC source (Vin) can be regenerated. Therefore, as a whole a DC-DC converter with high efficiency can be built.

FIG. 14 shows for information purposes the waveforms of the main waveforms measured in reality for the circuit shown above in FIG. 1. The switching devices and the parameters in this circuit are shown below.

-   -   auxiliary coil (Lw): 35 μH     -   resonant capacitor (Cw): 1 μF     -   main switching device (Qx): 2 SK 2843 (Toshiba)     -   auxiliary switching device (Qw): 2 SK 2843 (Toshiba)     -   main coil (Lx): 2.2 mH     -   fly-wheel diode (Dx): YG 1912S6 (Fujidenki)     -   smoothing capacitor (Cx): 0.47 μF     -   switching frequency: 100 kHz     -   load (Zx): 30 Ω     -   input voltage: 370 V     -   output wattage: 150 W     -   output voltage: 67 V     -   output current: 2.24 A

The advantage of one development of the first aspect of the invention is described below.

As is discussed above, in the circuit arrangement described above (FIG. 1), because the main switching device-gate driver signal (VxG) for driving the above described main switching device (Qx) and the auxiliary switching device-gate driver signal (VwG) for driving the auxiliary switching device (Qw) are activated in alternation, i.e., in an inverting manner, resonant operation is carried out.

Since, as is described above, current supply from the DC source (Vin) to the load side is carried out via the resonant capacitor (Cw), in the case of a small difference between the voltage of the DC source (Vin) and the output voltage of the DC-DC converter of the voltage reduction-buck type, the output current serviceability is reduced. For example, under these conditions, in the case in which amplification of the output current serviceability as the DC-DC converter becomes advantageous, it is necessary to switch the circuit arrangement such that current feed to the load side is not carried out via the resonant capacitor (Cw).

In the circuit arrangement of the invention the auxiliary switching device (Qw) is connected in parallel to the LC series connection in which the auxiliary coil (Lw) and the resonant capacitor (Cw) are connected in series. Therefore, by controlling the auxiliary switching device (Qw), resonant operation can be stopped easily by shifting the auxiliary switching device (Qw) into the ON state when the ON state of the main switching device (Qx) is reached.

FIG. 3 shows the situation for implementation of this by driving the main switching device (Qx) and the auxiliary switching device (Qw) in-phase in the circuit described above using FIG. 1. FIG. 3 shows the interval (Ton) during which the main switching device (Qx) is shifted into the ON state. The main switching device-gate driver signal (VxG) and the auxiliary switching device-gate driver signal (VwG) are operated so that the interval (Ton) is encompassed by an interval (Tw1) during which the auxiliary switching device (Qw) is shifted into the ON state. But a transition can also be carried out with the same timing.

FIG. 4 shows the situation in which resonant operation is likewise stopped by steady-state shifting of the auxiliary switching device (Qw) into the ON state.

Operation is simpler for the control shown in FIG. 4. However, the auxiliary switching device-gate driver signal (VwG) cannot be made direct-current, as in the case in which, for example, driving of the auxiliary switching device (Qw) using a pulse transformer is carried out. In the case in which the auxiliary switching device (Qw) cannot be shifted into the ON state in a steady-state manner, it is therefore advantageous to exercise control in the manner described above using FIG. 3.

With respect to the division of conditions for switching a state in which resonant operation is carried out, i.e., a resonance mode, and a state in which the resonant operation is stopped, i.e., a resonance stop mode, into one another, as was described above, it is possible to proceed as follows:

-   -   For example, as was described above, if the difference between         the voltage of the DC source (Vin) and the output voltage of the         DC-DC converter is small, the resonance stop mode is started.     -   In the other case there is a circuit by which for example the         continuity ratio of the main switching device (Qx) or an amount         which correlates to the continuity ratio is monitored for         control to achieve the resonance mode. Control can be exercised         in such a way that the resonance stop mode is started when it         has been determined that this continuity ratio is greater than         or equal to a predetermined value. Or there can simply be a         circuit by which the output voltage of the DC-DC converter is         monitored and control can be exercised such that the resonance         stop mode starts when it has been determined that this voltage         is greater than or equal to a predetermined value.

Furthermore it is also possible to proceed as follows:

Based on the property of the device to be used, as in the case of an application for the device described below for operating a discharge lamp, switching of the resonance mode and the resonance stop mode against one another can be carried out simply by time control based on the operation sequence when it is known, for example, beforehand that it is advantageous for there to be the resonance stop mode within a certain interval at the beginning.

The advantage of a second aspect of the invention is described below. As described in the prior art, the discharge voltage of a high pressure discharge lamp changes greatly and also vigorously depending on the discharge state, i.e., the state in which a no-load voltage is applied (state before the start of discharge), the glow discharge state, the state of a transient arc discharge, and the state of a steady-state arc discharge. Therefore, the converter for supply of a high pressure discharge lamp is required to have the property that enables a prompt change of the continuity ratio according to the discharge voltage of the high pressure discharge lamp in a wide, variable range with PWM control. Furthermore, there is a demand for a property that enables maintenance of operation in which the switching loss is reduced by resonance operation.

As described above, there is an auxiliary coil (Lw) of the circuit arrangement of the underlying DC-DC converter of the voltage reduction-buck type. Because the inductance of the auxiliary coil (Lw) is set intentionally smaller than the inductance of the main coil (Lx), the resonance phenomenon for the auxiliary coil (Lw) becomes less susceptible to the fluctuation of conditions at the load. Therefore, in a wide, variable range of the continuity ratio of the main switching device the switching loss can be reduced. It is therefore suited as a converter for supply of a high pressure discharge lamp. A device arranged using it therefore works advantageously for operating a high pressure discharge lamp.

FIG. 5 shows the circuit arrangement of a device for operating a high pressure discharge lamp (Ld) in a simplified representation in which the DC-DC converter for supplying a high pressure discharge lamp is the DC-DC converter of the voltage reduction-buck type of the invention, which was described above using FIG. 1.

To obtain a device for operating a high pressure discharge lamp (Ld), in addition to FIG. 1, there are a starter (Ui), a shunt resistor (R1) as the output current detector, voltage divider resistors (R2, R3) as the output voltage detectors and a feedback control element (Fb).

In the starter (Ui), a capacitor (Ci) is charged via a resistor (Ri) by a lamp voltage (VL). When a gate driver circuit (Gi) is activated, by closing the switching device (Qi) is comprised of a thyristor or the like, the capacitor (Ci) is discharged by the primary winding (Pi) of the transformer (Ti), by which in the secondary winding (Hi) a high voltage pulse is formed and applied between the electrodes (E1, E2) of the two poles of the high pressure discharge lamp (Ld). In this way, within the discharge space (Sd) an insulation breakdown occurs and the discharge of the high pressure discharge lamp (Ld) begins.

A lamp current determination signal (Sxi) is input by the shunt resistor (R1) and lamp voltage determination signals (Sxv) are input by the voltage divider resistors (R2, R3) to the feedback control element (Fb) from which a PWM signal (Sa) is sent to the driver control element (Gw). The driver control element (Gw) carries out drive control of the main switching device (Qx) and the auxiliary switching device (Qw) in this way.

The feedback control element (Fb) based on the lamp voltage determination signal (Sxv) before the start of discharge of the high pressure discharge lamp (Ld) carries out feedback control of the no-load voltage. That the starter (Ui) produces a high voltage pulse and that the discharge of the high pressure discharge lamp (Ld) has begun can be determined by the feedback control element (Fb), for example, by the lamp current determination signal (Sxi).

Furthermore the feedback control element (Fb) carries out the following:

-   -   The lamp wattage setpoint is divided by the lamp voltage value         which is computed by the lamp voltage determination signal         (Sxv);     -   In this way, the lamp current setpoint is computed at this         instant;     -   A lamp current setpoint signal that corresponds to this lamp         current setpoint is generated internally; and     -   Feedback control of the lamp current is carried out such that         the difference between it and the lamp current determination         signal (Sxi) is reduced.

However, as described above, since immediately after the transition into a transient arc discharge via a glow discharge, the lamp voltage is low and since the lamp current setpoint computed according to this lamp voltage value becomes unduly large, it is advantageous to exercise control so that the lamp current value is kept at the upper boundary value until finally the lamp voltage increases and until an appropriate lamp current setpoint is computed.

FIG. 6 shows one embodiment according to the first aspect of the invention. A version of a DC-DC converter of the invention is shown in which the auxiliary coil (Lw) and the resonant capacitor (Cw) are located downstream of the main switching device (Qx). Here the same action as in FIG. 1 can be used.

In the circuit arrangement shown in FIG. 6, a diode (Dw) is connected in parallel to the series connection of the auxiliary coil (Lw) and the main switching device (Qx) in order to avoid the following case.

There is specifically a case in which relatively great ringing arises at the electrical potential of the node of the nodal point between the main switching device (Qx) and the main coil (Lx) in the transition of the main switching device (Qx) into the ON state. When due to the presence of this ringing neither the disadvantage that for example the rated values of the switching devices are exceeded nor a similar disadvantage occurs, the diode (Dw) can also be omitted.

FIG. 7 shows one embodiment of the first aspect of the invention.

Here, an embodiment of a DC-DC converter of the invention is shown, in which the auxiliary coil (Lw) is located on a line (ground line) of the DC source (Vin) which is opposite the line on which the main switching device (Qx) and the main coil (Lx) are located next to one another. Here the same action as in FIG. 1 can be used.

FIG. 8 shows the arrangement of the driver control element (Gw) and the feedback control element (Fb) of a DC-DC converter of the invention in a simplified representation.

The feedback control element (Fb) comprises the following:

-   -   an arithmetic circuit (Uj) which computes the lamp current         setpoint by dividing the lamp wattage setpoint by a lamp voltage         value which is computed on the basis of lamp voltage         determination signal (Sxv),     -   a driving capacity control circuit (Ud) which carries out pulse         width modulation with feedback such that the difference between         the lamp current setpoint signal (Sbv) which has been computed         by this arithmetic circuit (Uj) and the lamp current         determination signal (Sxi) is reduced at this time; and     -   a resonance control circuit (Uc) which generates a resonance         prohibition signal (Sc) which is used to switch the resonance         mode and the resonance stop mode into one another and which         prohibits resonant operation.

The PWM signal (Sa) is output by the driving capacity control circuit (Ud).

Here, if the resonance prohibition signal (Sc) is inactive, the main switching device (Qx) and the auxiliary switching device (Qw) must be shifted in alternation into the ON state. Therefore the main switching PWM signal (Sax) which is to become a driver signal of the main switching device (Qx) and the auxiliary switching PWM signal (Saw) which is to become an inversion signal of it, i.e., a driver signal of the auxiliary switching device (Qw), are generated. If conversely the resonance prohibition signal (Sc) is activated, the auxiliary switching PWM signal (Saw) is generated as an in-phase signal with respect to the main switching PWM signal (Sax) or as a signal which shifts the auxiliary switching device (Qw) into the ON state in a steady-state manner.

This generation of the auxiliary switching PWM signal (Saw) with respect to the main switching PWM signal (Sax) in an inverting, in-phase or steady-state manner takes place in a signal conversion part (Uf) when the resonance prohibition signal (Sc) is received. The generated main switching PWM signal (Sax) and the generated auxiliary switching PWM signal (Saw) are converted at the driver control element (Gw) into signals which are used to drive the switching devices.

Since control is exercised in such a way that only after the auxiliary switching device (Qw) reaches the OFF state is the main switching device (Qx) shifted into the ON state within a given time, this time can be regulated by adding a delay circuit (Un) for delaying the timing for driving the main switching device (Qx).

Next, there are circuits for driving the main switching device (Qx) and the auxiliary switching device (Qw), for example driver circuits (Uqx, Uqw) comprised of a pulse transformer, a high-side-driver or the like. In this way, driver signals (Sqx, Sqw) are generated for the respective switching device and the respective switching device is subjected to ON-OFF control.

A microprocessor (not shown in the drawings) can be installed in the feedback control element (Fb) and thus the discharge state of the high pressure discharge lamp can be identified and a relatively complicated sequence which is subject to normal operation control can be processed. Here, it is advantageous to proceed as follows:

-   -   The lamp voltage determination signal (Sxv) is converted by AD         conversion into a lamp voltage value.     -   The computation of the lamp current setpoint which satisfies a         lamp wattage setpoint is done by the microprocessor.     -   A lamp current setpoint signal is generated by a D/A converter.

FIG. 9 shows an embodiment of part of the feedback control element (Fb) of the invention and of the circuit arrangement of the driver control element (Gw) of a DC-DC converter.

In the driving capacity control circuit (Ud), the error of the lamp current determination signal (Sxi) at this time is integrated with respect to the lamp current setpoint signal (Sbv) using an error integrator which consists of a capacitor (Cp) and an operational amplifier (Ade). The integrated integration signal (Sd1) is compared using a comparator (Cmg) to a sawtooth wave which has been produced in an oscillator for producing sawtooth waves (Osc). In this way the PWM signal (Sa) is generated such that a signal is obtained for which the magnitude of the continuity ratio changes according to the magnitude of the integration signal (Sd1), i.e., a driver signal is obtained which is subjected to PWM control for the main switching device (Qx).

In FIG. 9, for the resonance control circuit (Uc) the magnitude of the integration signal (Sd1) is compared to the signal of a reference voltage signal generator (Vtc) using a comparator (Cmc), thus it is assessed whether a state is present or not in which the integration signal (Sd1) produces a continuity ratio which is greater than a given value, and the resonance prohibition signal (Sc) is generated such that when the integration signal (Sd1) produces a continuity ratio which is greater than a given value, the resonance prohibition mode is entered and that in the other case the resonance mode is entered.

FIG. 9 describes a case in which the gate signal of the auxiliary switching device (Qw) is generated using the pulse transformer (Tw). When the resonance prohibition signal (Sc) of the resonance prohibition mode is chosen, the auxiliary switching device (Qw) is therefore not shifted into the ON state in a steady-state manner, but is driven in-phase with the main switching device (Qx).

In the resonance mode, with the gate signal of the auxiliary switching device (Qw), the main switching device (Qx) and the auxiliary switching device (Qw) are shifted alternately into the ON state. Therefore, the PWM signal (Sa) and an inversion signal of it are required. Conversely, in the resonance prohibition mode a signal for which the PWM signal (Sa) has been inverted is not necessary.

Therefore, there is a buffer (Bx) which with respect to the above described PWM signal (Sa) produces the above described in-phase main switching PWM signal (Sax) (noninverting, installed if necessary). Furthermore there is an inverter (Bw) which generates an inversion signal of it. Using a data switch (Se1) and based on the above described resonance prohibition signal (Sc), a signal is chosen and sent to the rear stage as the above described auxiliary switching PWM signal (Saw) for producing the gate signal of the above described auxiliary switching device (Qw).

In doing so, the main switching PWM signal (Sax) is output via a buffer (Bfx) to the next stage, since a delay circuit is formed which follows the time constant of a CR circuit consisting of a resistor (Rx2) and a capacitor (Cx1). In this delay circuit, a delay can be taken to a sufficient extent in the case of reaching “High”. Conversely, in the case in which the voltage of the buffer (Bfx) drops from “High” to “Low”, control is exercised in such a way that parallel to the resistor (Rx2) a diode (Dx1) is added, an electrical charge is quickly withdrawn from the capacitor (Cx1) and thus the delay time is shortened. Thus, only the signal of when the main switching device (Qx) is turned on is delayed.

Then, the signal which has been output from the buffer (Bfx) is transmitted via a base resistor (Rx3) to a driver circuit (Uqx) for driving the main switching device (Qx). From the nodal point between the driver circuit (Uqx) and the switching devices (Qx2, Qx3), a signal is transmitted to the primary winding (Px) of the pulse transformer (Tx) via a capacitor (Cx2) and a resistor (Rx4) as the current limitation resistor. A resistor (Rx5) which is to become the gate resistor of the main switching device (Qx) is connected from the secondary winding (Sx) of the pulse transformer (Tx). A resistor (Rx6) is connected thereto and is connected between the drain and the source electrode in order to smoothly turn off the main switching device (Qx). These signals (Sqx1, Sqx2) are transmitted to the main switching device (Qx).

On the other hand, a delay is added to the auxiliary switching PWM signal (Saw) by a delay circuit (Um) which likewise consists of a resistor (Rw2), a capacitor (Cw1), a diode (Dw1) and a buffer (Bfw). The signal which has been output via the buffer (Bfw) is transmitted to the switching devices (Qw2, Qw3) via the base resistor (Rw4) and proceeds from the nodal point between the switching devices (Qw2, Qw3) via a capacitor (Cw2) and a resistor (Rw7) as a current limitation resistor to the primary winding (Pw) of the pulse transformer (Tw). A gate resistor (Rw5) of the auxiliary switching device (Qw) and a resistor (Rw6) which is connected between the drain and the source electrode is connected to the secondary winding (Sw) for smoothly turning off the auxiliary switching device (Qw). Generated driver signals (Sqw1, Sqw2) are transmitted to the auxiliary switching device (Qw).

By this arrangement, in the control circuit shown in FIG. 9, the device of the invention for operating a high pressure discharge lamp can be controlled with feedback such that the error between the lamp current determination signal (Sxi) and the lamp current setpoint signal (Sbv) decreases. Under the condition under which the continuity ratio of the main switching device (Qx) is smaller than a given value, i.e., under which the output voltage is relatively low, a resonance mode can be achieved and the main switching device (Qx) and the auxiliary switching device (Qw) can be subjected to ON-OFF control in such a way that the switching loss is reduced. Conversely, under the condition under which the continuity ratio of the main switching device (Qx) is greater than a given value, i.e., under which the output voltage is relatively high, a resonance stop mode is obtained and the same output current serviceability as in a conventional DC-DC converter of the voltage reduction-buck type is ensured.

In the resonance mode for the main switching PWM signal (Sax) and the auxiliary switching PWM signal (Saw) for the two switching devices, specifically for the main switching device (Qx) and the auxiliary switching device (Qw), there are delay circuits (Un, Um). In this way, the switching devices are prevented from being turned on at the same time.

In this embodiment, the integration signal (Sd1) is monitored as an amount correlating to the continuity ratio of the main switching device (Qx). Control is exercised such that in the case of a large continuity ratio the resonance stop mode starts. This control process is very well suited as a DC-DC converter for a device for operating a discharge lamp.

The reason for this is the following:

As was described above, in the state in which a no-load voltage with a high output voltage is applied, no output current flows. In a glow discharge likewise with a high output voltage the output current is far smaller than in an arc discharge. Under the condition under which these output voltages are high, the wattage supplied to the load is therefore originally small. The loss in the main switching device (Qx) is therefore low. Therefore an increase of the loss by the starting of the resonance stop mode can be ignored for the most part.

For example, TL494 from Texas Instruments or the like can be used as a commercial IC in which functional units such as the operational amplifier (Ade) described above using FIG. 9, the oscillator shown in FIG. 9 for producing sawtooth waves (Osc), the comparator (Cmg) shown in FIG. 9 for comparison with the sawtooth waves and the like are integrated.

FIG. 10 shows an embodiment according to the second aspect of the invention. This embodiment is a device for operating a high pressure discharge lamp using a starter which is called an external trigger type. In the high pressure discharge lamp (Ld), there is an auxiliary electrode (Et) besides the electrodes for the main discharge such that it does not come into contact with the discharge space (Sd). Between this auxiliary electrode (Et) and the first and second electrodes, a high voltage is applied, by which plasmas are produced in the discharge space (Sd). The main discharge is started by a voltage (no-load voltage) that is applied beforehand between the first electrode and the second electrode, with the plasmas acting as the initiating substance.

FIG. 11 shows an embodiment according to the second aspect of the invention. Here, a device for operating a high pressure discharge lamp of the external trigger type is shown in which an AC voltage is applied to the high pressure discharge lamp (Ld).

It is possible to apply an alternating discharge voltage to the high pressure discharge lamp (Ld) by installing a full bridge inverter. The full bridge inverter is obtained by adding switching devices to the DC output part of the DC-DC converter. The added switching devices are driven by a control circuit part (Gf) for full bridge driving and are controlled in such a way that the diagonal elements are driven in alternation so that the switching devices (Q1, Q4) (Q2, Q3) are closed at the same time as the diagonal elements of the full bridge inverter.

FIG. 12 shows a schematic of the state of the lamp voltage (VL), of the lamp current (IL) and of the resonance prohibition signal (Sc) according to one embodiment of the second aspect of the invention.

An embodiment was described above in which the integration signal (Sd1) is monitored as the amount which correlates to the continuity ratio of the main switching device (Qx) and in which control is exercised such that in the case of a large continuity ratio the resonance stop mode is started. Subsequently, one embodiment in an even more simplified representation is shown in which the resonance stop mode and afterwards the resonance mode begin from the starting of the discharge lamp until a given time expires.

In FIG. 12, during the interval (τv) a no-load voltage (Vs) is output. FIG. 12 shows a situation in which at the time (τg) the starter is operated, in which during an interval (τg) a glow discharge with a certain glow discharge voltage (Vg) forms, and in which afterwards an arc discharge is formed. However, in fact, there is also a case in which a transition to an arc discharge takes place once, in which a return to a glow discharge occurs, in which in the case of a transition again to an arc discharge the extinction of the discharge takes place when the glow discharge returns and in which proceeding from the output of the no-load voltage a repeated attempt is made. After expiration of the interval during which a transition phenomenon such as a glow discharge, extinction of the discharge and the like, occurs, the transition into the arc discharge is completed.

Since the lamp voltage is low during the interval (τe) immediately after completion of the transition into the arc discharge, the lamp current becomes unduly large when an attempt is made to supply the rated wattage to the lamp during this interval. The lamp current is limited to a suitable current value of the upper limit (Ic) and output is carried out. During this interval (τe) therefore a wattage which is lower than the rated wattage is applied to the lamp.

The interval during which the transition phenomenon occurs is restricted to a limited time. Expressed in greater detail, such a transition phenomenon is generally continued when the interval during which the lamp is off is short after completion of lamp operation when the lamp temperature is too high. This repeated induction of such a transition phenomenon shortens the lamp service life. When the transition into the arc discharge is not completed within a given interval, for purposes of lamp protection the attempt to operate the lamp is stopped. As a result the interval during which the transition phenomenon occurs is restricted to a limited time. When the lamp temperature is low enough, the transition into the arc discharge is of course in fact completed within the given interval.

As described above, under the condition under which a high voltage is output, as in a glow discharge, the resonance stop mode can be started. As discussed, the interval during which the resonance stop mode is to be started is restricted to a limited time. It is therefore relatively practical to exercise control in the following manner.

A suitable interval is established without the confirmation of whether in fact a glow discharge takes place or not. Within this interval, the resonance stop mode is started after initiating the start-up of the lamp and the resonance mode is started after this interval expires.

A case was described above using FIG. 12 in which within an interval (τr) after the beginning of start-up of the lamp the resonance prohibition signal (Sc) is activated, in which the resonance stop mode is started, and in which the resonance mode is started after this interval expires. However, in FIG. 12, a polarity is assumed for which the resonance stop mode is started when the resonance prohibition signal (Sc) is at a high level.

The interval (πr) will be fixed in the following manner:

It should be greater than the interval during which a transition phenomenon such as the glow discharge, the extinction of the discharge and the like, can occur. But it should be shortened to the extent that it does not exceed the end of the interval (πe) during which a wattage lower than the rated wattage is supplied to the lamp.

FIG. 13 shows one embodiment of part of a feedback control element (Fb) of the invention and the circuit arrangement of the driver control element (Gw) of a DC-DC converter. In this arrangement the auxiliary switching device (Qw) is shifted into the ON state when the resonance prohibition signal (Sc) is at a low level.

The delay circuits (Un, Um) and the driver circuit (Uqx) were described above using the embodiment described in FIG. 9.

For the gate signal of the auxiliary switching device (Qw), the main switching device (Qx) and the auxiliary switching device (Qw) are shifted in alternation into the ON state. Therefore the PWM signal (Sa) and an inversion signal thereof are needed. Therefore, with respect to the PWM signal (Sa) there are two switching devices (Qx1, Qw1). The switching device (Qx1) is an emitter follower by a resistor (Rx1) and generates a main switching PWM signal (Sax) which is an in-phase signal like the PWM signal (Sa). A resistor (Rw1) is connected to the switching device (Qw1). Furthermore the switching device (Qw1) is an emitter ground and generates an auxiliary switching PWM signal (Saw) which is an inversion signal with respect to the PWM signal.

In the signal conversion part (Uf), the auxiliary switching PWM signal (Saw), which will become the driver signal of the auxiliary switching device (Qw), is generated. When the resonance prohibition signal (Sc) is at a low level, the switching device (Qc) is shifted into the ON state and the switching device (Qw1) is shifted into the OFF state via a resistor (Rw0) which is connected in series to a resistor (Rx0). As a result the auxiliary switching PWM signal (Saw) reaches a high level, passes through the delay circuit (Um) and is transmitted to the driver circuit (Uqw).

Since it is difficult using a pulse transformer to shift the auxiliary switching device (Qw) into the ON state in a steady-state manner, it is necessary to use an insulation means such as a high-side-driver, a photocoupler or the like. If the auxiliary switching device (Qw) is a FET, it is necessary to connect the source terminal to the ground of the driver control element (Gw).

The driver circuit described above using FIG. 13 is an example in which a high-side-driver (Hsd) is used which comprises a signal generator (Hsc) and switching devices (QH, QL) that can directly drive the auxiliary switching device (Qw), and the like. The voltage which becomes the current source of the output of this high-side-driver (Hsd) is subjected to a “charge pump up” by an arrangement of a capacitor (Ch) and a diode (Dh) by the ON-OFF of the main switching device (Qx). In the capacitor (Ch), a current source for driving the auxiliary switching device (Ow) is produced.

The auxiliary switching PWM signal (Saw) passes through the delay circuit (Um), passes through the high-side-driver (Hsd) and is output via a resistor (Rh). The output here is at a high level. The generated driver signals (Sqw1, Sqw2) are transmitted to the auxiliary switching device (Qw) with a high voltage. Resonance operation can be easily switched by this arrangement by the resonance prohibition signal (Sc).

In the DC-DC converter of the invention zero voltage switching is accomplished in the transition of the auxiliary switching device (Qw) into the ON state. Therefore the occurrence of noise can also be kept fundamentally low during this switching.

In these application documents, only what is most necessary in the circuit arrangement is described in order to explain the operation, function and action of the light source device of the invention. It is therefore assumed that the other details of circuit operation which is described in the embodiments, for example, the polarity of the signals, the specific choice, the specification addition and omission of circuit components or concepts such as changes and the like are intensively carried out for reasons of facilitating the procurement of components and for economic reasons, in the practice of building an actual device.

It is assumed that especially a device for protecting the circuit components of a feed device, such as switching devices such as a FET or the like, against damage factors such as a wattage which exceeds a certain value, a current which exceeds a certain value, overheating and the like, or a device which reduces formation of radiation noise and line noise that arise according to operation of the circuit components of the feed device, or which prevents the noise formed from being released to the outside, such as a snubber circuit, a varistor, a clamping diode (including the “pulse-by-pulse method”), a current limiter circuit, a noise filter reactor coil with a “common mode” or a “normal mode”, a noise filter capacitor and the like if necessary is added to the respective part of the circuit arrangements which are described in the embodiments.

The invention according to the first aspect can provide a DC-DC converter by which the disadvantage of a conventional DC-DC converter, i.e., the disadvantage of difficult implementation of reducing the switching loss in a wide variable range of the continuity ratio of the main switching device with low costs, is eliminated.

The invention according to the second aspect can provide a device for operating a high pressure discharge lamp by which the disadvantage of a conventional device for operating a high pressure discharge lamp, i.e., the disadvantage of difficult implementation of reducing the switching loss with low costs, is eliminated. 

1. A DC-DC converter of the voltage reduction-buck type comprising: a direct current source (Vin); an ON-OFF-controllable main switching device (Qx); a main coil (Lx) in series connection to the main switching device (Qx); a fly-wheel diode (Dx) operatively arranged so that the induction current of the main coil (Lx) flows when the main switching device (Qx) is shifted into the OFF state; a smoothing capacitor (Cx) for smoothing the output of the main coil (Lx); an auxiliary coil (Lw); a resonant capacitor (Cw); and an ON-OFF-controllable auxiliary switching device (Qw), wherein the auxiliary coil (Lw) and the resonant capacitor (Cw) are series-connected to form a LC series connection, wherein the LC series connection, the main switching device (Qx) and the fly-wheel diode (Dx) are series connected, wherein the auxiliary switching device (Qw) is connected in parallel to the LC series connection, and wherein the main switching device (Qx) and the auxiliary switching device (Qw) are controlled such that they are alternatively shifted into the ON state, and the main switching device (Qx) is shifted into the ON state within a given time after the auxiliary switching device (Qw) has been shifted into the OFF state.
 2. The DC-DC converter as set forth in claim 1, wherein when in the state in which a resonance prohibition signal (Sc) is activated and when the ON state of the main switching device (Qx) is reached, the auxiliary switching device (Qw) also is shifted into the ON state, instead of the main switching device (Qx) and the auxiliary switching device (Qw) being controlled such that they are alternatively shifted into the ON state and the main switching device (Qx) being shifted into the ON state within a given time after the auxiliary switching device (Qw) has been shifted into the OFF state.
 3. A device for operating a high pressure discharge lamp (Ld) in which a discharge space (Sd) is filled with a discharge medium and an opposed pair of electrodes (E1, E2) for the main discharge are positioned within the discharge space, the device comprising the DC-DC converter of claim
 1. 4. A device for operating a high pressure discharge lamp (Ld) in which a discharge space (Sd) is filled with a discharge medium and an opposed pair of electrodes (E1, E2) for the main discharge are positioned within the discharge space, the device comprising the DC-DC converter of claim
 2. 